An axion is a hypothetical particle proposed as a candidate for dark matter.The axion is a light particle predicted to solve the problem of CP violation in the strong interaction (why quarks behave symmetrically under mirror reflection). It hardly interacts with matter and could constitute cold dark matter. The search is conducted by attempting to convert an axion into a photon under the influence of a strong magnetic field.
The Peccei-Quinn mechanism was published in 1977, and soon Frank Wilczek and Steven Weinberg independently predicted a light boson. Wilczek named it the axion, by analogy with a cleaning agent that 'cleans up' QCD from the strong CP problem. In the 1980s, the first experiments were proposed, including a 'magnetic sequester.' In the 21st century, axion searches have become one of the main directions of particle physics, intertwined with astrophysics and cosmology.
The axion field a(x) interacts with electromagnetism through the term (g_{aγγ}/4) a F_{μν} ilde{F}^{μν} in the Lagrangian. In an external magnetic field, this leads to the conversion of axions into photons. Cosmologically, axions are born at the spontaneous breaking of symmetry, and their field is frozen until the moment when the mass becomes comparable to the Hubble rate; then it begins to oscillate, behaving as cold dark matter. For detection, resonance in microwave cavities is used (frequency is related to the axion mass) with sensitivity g_{aγγ} ~ 10^{-16} GeV^{-1}.
The search for axions is underway in dozens of laboratories using sensitive detectors and powerful magnets; their discovery will decipher the nature of dark matter and open the way to new physics.
An axion could shine through a solid lead wall a light-year thick without even noticing it.
| l_osc | variable | Oscillation length — length metre |
| E_c | variable | Critical energy — energy joule |
| E_γ | variable | Photon energy — energy joule |
| B_perp | variable | Perpendicular magnetic field strength — magnetic field strength tesla |
| g_aγ | variable | Axion-photon coupling constant — coupling constant inverse gev |
| q | variable | Axis ratio — axis ratio |
| Z | variable | Height (vertical extent) — length metre |
| X | variable | Length (horizontal extent) — length metre |
| m_a | variable | Axion mass — mass kilogram |
| f_a | variable | Axion decay constant (symmetry breaking scale) — energy joule |
| ∝ | operator | Indicates a direct proportionality relationship — proportionality |
| z | variable | Input vector to be projected — vector |
| p | variable | Projected vector on the simplex — vector |
| proj | operator | Finds the closest point in the simplex to the input vector — projection operator |
| argmin | operator | Returns the value that minimizes the expression — argmin operator |
| ‖·‖ | operator | Computes the square root of the sum of squares — euclidean norm |
| \theta_{a,0} | variable | Amplitude of polarization oscillation — angle radian |
| g_{a\gamma} | variable | Axion-photon coupling constant — coupling constant reciprocal gev |
| \rho | variable | Local axion dark matter density — mass density kilogram per cubic metre |
| \mu | variable | Axion mass — mass kilogram |














